2021
DOI: 10.1016/j.solmat.2021.111172
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Detection of stable positive fixed charges in AlOx activated during annealing with in situ modulated PhotoLuminescence

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Cited by 5 publications
(7 citation statements)
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“…During the hydrogenation processes in the MVS PECVD chamber (annealing, a‐SiN x :H deposition, NH 3 + H 2 plasma treatment), the minority carrier lifetime was monitored by an in situ MPL measurement setup mounted on the PECVD reactor, similar to the one described in a previous article. [ 9,16 ] The MPL characterization technique consists in shining a sample with a modulated laser intensity (excitation wavelength of 785 nm), which induces a modulation of the photoluminescence signal. By measuring the phase shift ϕ $\phi $ between this MPL signal and the excitation, the differential minority carrier lifetime τnormalm ${\tau }_{{\rm{m}}}$ can be determined through the equation given below [ 8 ] : ϕ=arctan (ωτnormalm), $\phi =-\text{arctan}\unicode{x02007}(\omega {\tau }_{{\rm{m}}}),$where ω $\omega $ is the pulsation of the modulation of the laser in rad s −1 .…”
Section: Methodsmentioning
confidence: 99%
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“…During the hydrogenation processes in the MVS PECVD chamber (annealing, a‐SiN x :H deposition, NH 3 + H 2 plasma treatment), the minority carrier lifetime was monitored by an in situ MPL measurement setup mounted on the PECVD reactor, similar to the one described in a previous article. [ 9,16 ] The MPL characterization technique consists in shining a sample with a modulated laser intensity (excitation wavelength of 785 nm), which induces a modulation of the photoluminescence signal. By measuring the phase shift ϕ $\phi $ between this MPL signal and the excitation, the differential minority carrier lifetime τnormalm ${\tau }_{{\rm{m}}}$ can be determined through the equation given below [ 8 ] : ϕ=arctan (ωτnormalm), $\phi =-\text{arctan}\unicode{x02007}(\omega {\tau }_{{\rm{m}}}),$where ω $\omega $ is the pulsation of the modulation of the laser in rad s −1 .…”
Section: Methodsmentioning
confidence: 99%
“…This study lead to the observation of the activation of positive fixed charges in Al 2 O 3 under the combined action of light and temperature. [9] In the present work, we investigate the possibility to use a simplified process flow for the fabrication of FPC samples, in a way close to the one proposed by Ingenito et al [10] As shown in Figure 1b and detailed in a previous communication, it consists in depositing sequentially a stack of silicon oxide (SiO x )/(p) nanocrystalline silicon (nc-Si:H)/a-SiN x :H and making a final firing step. [7] The tunnel SiO x layer provides chemical passivation to the surface of the wafer while allowing the transport of charge carriers by diffusion through pinholes or tunneling; the doped nc-Si:H layer has the role of a carrier-selective contact (conductivity, band bending).…”
Section: Introductionmentioning
confidence: 98%
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“…AlO x is also shown to have positive fixed charges when annealed at low temperature under light. [ 96 ] The deposition was at 150 °C in this case. Recently, a combined stack of PO x and AlO x revealed very high Q f between 10 12 and 10 13 e cm −2 and D it of 10 10 eV −1 cm −2 for as‐deposited layers.…”
Section: Outlook For Dielectric Front Passivationmentioning
confidence: 99%
“…By taking advantage of the negative fixed charge density of AlO x itself, a passivation with surface recombination velocity (SRV) close to 10 cm/s has been achieved for p-type silicon [10]. Two main approaches have been developed to improve the passivation quality provided by AlO x including thermal annealing [11][12][13][14] and light-soaking [15][16][17].…”
Section: Introductionmentioning
confidence: 99%